{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:MSFLPGD5HQRNZLZLMVWN37SOCM","short_pith_number":"pith:MSFLPGD5","canonical_record":{"source":{"id":"2101.08105","kind":"arxiv","version":6},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-01-20T13:07:14Z","cross_cats_sorted":[],"title_canon_sha256":"0f708c6a49015572c87fc401fde23c82c3f2e36df545d2ab143aefee642b0f14","abstract_canon_sha256":"2c7cadda574d406d53ff03f4eb7094bd9b670a0049b4740ec5be1fae1c16290b"},"schema_version":"1.0"},"canonical_sha256":"648ab7987d3c22dcaf2b656cddfe4e13234f885ddefb18a45ae4d29b1c32382d","source":{"kind":"arxiv","id":"2101.08105","version":6},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2101.08105","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"arxiv_version","alias_value":"2101.08105v6","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.08105","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_12","alias_value":"MSFLPGD5HQRN","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_16","alias_value":"MSFLPGD5HQRNZLZL","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_8","alias_value":"MSFLPGD5","created_at":"2026-07-05T07:37:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:MSFLPGD5HQRNZLZLMVWN37SOCM","target":"record","payload":{"canonical_record":{"source":{"id":"2101.08105","kind":"arxiv","version":6},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-01-20T13:07:14Z","cross_cats_sorted":[],"title_canon_sha256":"0f708c6a49015572c87fc401fde23c82c3f2e36df545d2ab143aefee642b0f14","abstract_canon_sha256":"2c7cadda574d406d53ff03f4eb7094bd9b670a0049b4740ec5be1fae1c16290b"},"schema_version":"1.0"},"canonical_sha256":"648ab7987d3c22dcaf2b656cddfe4e13234f885ddefb18a45ae4d29b1c32382d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:37:27.016601Z","signature_b64":"8oEWNkEaqzcjYJcCRYEra+6KEf1tjUd5lqIupWq0IiwxuxiKUobRwx0V2Ygj5lydrU/Zj9XLsd2siaIy69jnBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"648ab7987d3c22dcaf2b656cddfe4e13234f885ddefb18a45ae4d29b1c32382d","last_reissued_at":"2026-07-05T07:37:27.016193Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:37:27.016193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2101.08105","source_version":6,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T07:37:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WhVJiSff/bRMinRogQJ0xbmDG+r4JfMnTyxb/37UZwabBoXnX6j0k+PEkuBBrmMGwhp/oawuMTjXKYio83LRBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T21:45:41.066762Z"},"content_sha256":"9997c197169945bb8c0f3510f4b8f201b5f430d6b5c6045e67aba7030aef92c9","schema_version":"1.0","event_id":"sha256:9997c197169945bb8c0f3510f4b8f201b5f430d6b5c6045e67aba7030aef92c9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:MSFLPGD5HQRNZLZLMVWN37SOCM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic Schwinger Effect in Anisotropic Media","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jialun Ping, Jing Zhou, Jun Chen, Le Zhang, Xun Chen","submitted_at":"2021-01-20T13:07:14Z","abstract_excerpt":"According to gauge/gravity correspondence, we study the holographic Schwinger effect within an anisotropic background. Firstly, the separate length of the particle-antiparticle pairs is computed within the context of an anisotropic background which is parameterized by dynamical exponent $\\nu$. It is found that the maximum separate length $x$ increases with the increase of dynamical exponent $\\nu$. By analyzing the potential energy, we find that the potential barrier increases with the dynamical exponent $\\nu$ at a small separate distance. This observation implies that the Schwinger effect with"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.08105","kind":"arxiv","version":6},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2101.08105/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T07:37:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/B2aFfAkVZrfoz611t6hU2GwijWvwp60u256yv0xUAglbUsebV5X+cuQvbIHBVuUwrRQmkftZXNJyO9JNlIyCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T21:45:41.067278Z"},"content_sha256":"db1cc1f0fbd2ec3a53403abad82caeb58f2871cb76aae9649fa28ebeb6bfd3fc","schema_version":"1.0","event_id":"sha256:db1cc1f0fbd2ec3a53403abad82caeb58f2871cb76aae9649fa28ebeb6bfd3fc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/bundle.json","state_url":"https://pith.science/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-08T21:45:41Z","links":{"resolver":"https://pith.science/pith/MSFLPGD5HQRNZLZLMVWN37SOCM","bundle":"https://pith.science/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/bundle.json","state":"https://pith.science/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MSFLPGD5HQRNZLZLMVWN37SOCM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:MSFLPGD5HQRNZLZLMVWN37SOCM","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"2c7cadda574d406d53ff03f4eb7094bd9b670a0049b4740ec5be1fae1c16290b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-01-20T13:07:14Z","title_canon_sha256":"0f708c6a49015572c87fc401fde23c82c3f2e36df545d2ab143aefee642b0f14"},"schema_version":"1.0","source":{"id":"2101.08105","kind":"arxiv","version":6}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2101.08105","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"arxiv_version","alias_value":"2101.08105v6","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.08105","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_12","alias_value":"MSFLPGD5HQRN","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_16","alias_value":"MSFLPGD5HQRNZLZL","created_at":"2026-07-05T07:37:27Z"},{"alias_kind":"pith_short_8","alias_value":"MSFLPGD5","created_at":"2026-07-05T07:37:27Z"}],"graph_snapshots":[{"event_id":"sha256:db1cc1f0fbd2ec3a53403abad82caeb58f2871cb76aae9649fa28ebeb6bfd3fc","target":"graph","created_at":"2026-07-05T07:37:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2101.08105/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"According to gauge/gravity correspondence, we study the holographic Schwinger effect within an anisotropic background. Firstly, the separate length of the particle-antiparticle pairs is computed within the context of an anisotropic background which is parameterized by dynamical exponent $\\nu$. It is found that the maximum separate length $x$ increases with the increase of dynamical exponent $\\nu$. By analyzing the potential energy, we find that the potential barrier increases with the dynamical exponent $\\nu$ at a small separate distance. This observation implies that the Schwinger effect with","authors_text":"Jialun Ping, Jing Zhou, Jun Chen, Le Zhang, Xun Chen","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-01-20T13:07:14Z","title":"Holographic Schwinger Effect in Anisotropic Media"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.08105","kind":"arxiv","version":6},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:9997c197169945bb8c0f3510f4b8f201b5f430d6b5c6045e67aba7030aef92c9","target":"record","created_at":"2026-07-05T07:37:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"2c7cadda574d406d53ff03f4eb7094bd9b670a0049b4740ec5be1fae1c16290b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-01-20T13:07:14Z","title_canon_sha256":"0f708c6a49015572c87fc401fde23c82c3f2e36df545d2ab143aefee642b0f14"},"schema_version":"1.0","source":{"id":"2101.08105","kind":"arxiv","version":6}},"canonical_sha256":"648ab7987d3c22dcaf2b656cddfe4e13234f885ddefb18a45ae4d29b1c32382d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"648ab7987d3c22dcaf2b656cddfe4e13234f885ddefb18a45ae4d29b1c32382d","first_computed_at":"2026-07-05T07:37:27.016193Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:37:27.016193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8oEWNkEaqzcjYJcCRYEra+6KEf1tjUd5lqIupWq0IiwxuxiKUobRwx0V2Ygj5lydrU/Zj9XLsd2siaIy69jnBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:37:27.016601Z","signed_message":"canonical_sha256_bytes"},"source_id":"2101.08105","source_kind":"arxiv","source_version":6}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9997c197169945bb8c0f3510f4b8f201b5f430d6b5c6045e67aba7030aef92c9","sha256:db1cc1f0fbd2ec3a53403abad82caeb58f2871cb76aae9649fa28ebeb6bfd3fc"],"state_sha256":"a09e6ac594d0549d7809518a19e0c6775750615d7fc3199f8687539456029129"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4nLJAcIvwZ70nVavjeFK4fs7uMqhD2OQl1bFCYM8CJbrJgSkrlYFE0NrRalIiD5HeV/cXcLSxl3rdEynYCG1Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T21:45:41.072287Z","bundle_sha256":"fb9566514fd326bc52fc2a64b401dbf69c8a7029ab21a2155fad1678be9fbc7e"}}